Test case HOM12: Rotating turbulence with axisymmetric strain, data from Leuchter & Dupeuble (1993)

Table 3:  Duct 2 (L=0.5 m),  Omega0/D=0


The results are displayed in a table with 8 columns corresponding to the
following quantities:

 - longitudinal position x (m),

 - local strain rate D (s^-1), evaluated from D=dU/dx

 - local rotation rate Omega (rd/s), evaluated from Omega=Omega_0.U/U_0,

 - axial mean velocity component U (m/s),

 - Reynolds stresses u^2, v^2 (m^2/s^2),

 - trace of the Reynolds stress tensor q^2 (m^2/s^2), evaluated from q^2=u^2+2.v^2,

 - dissipation rate epsilon (m^2/s^3), evaluated from epsilon=-D(u^2-v^2)-1/2.U.dq^2/dx.


     x            D         Omega         U           u^2         v^2         q^2       epsilon 
    (m)         (s^-1)      (rd/s)      (m/s)      (m^2/s^2)   (m^2/s^2)   (m^2/s^2)   (m^2/s^3) 

 -0.1250E+00   0.000E+00   0.000E+00   0.808E+01   0.501E+00   0.291E+00   0.108E+01   0.510E+02
 -0.9375E-01   0.126E+01   0.000E+00   0.805E+01   0.331E+00   0.196E+00   0.722E+00   0.345E+02
 -0.6250E-01   0.624E+01   0.000E+00   0.817E+01   0.237E+00   0.144E+00   0.524E+00   0.211E+02
 -0.3125E-01   0.142E+02   0.000E+00   0.847E+01   0.159E+00   0.113E+00   0.386E+00   0.127E+02
  0.0000E+00   0.229E+02   0.000E+00   0.906E+01   0.126E+00   0.927E-01   0.311E+00   0.832E+01
  0.3125E-01   0.312E+02   0.000E+00   0.989E+01   0.963E-01   0.822E-01   0.261E+00   0.596E+01
  0.6250E-01   0.385E+02   0.000E+00   0.110E+02   0.769E-01   0.739E-01   0.225E+00   0.451E+01
  0.9375E-01   0.426E+02   0.000E+00   0.123E+02   0.646E-01   0.696E-01   0.204E+00   0.366E+01
  0.1250E+00   0.450E+02   0.000E+00   0.136E+02   0.542E-01   0.678E-01   0.190E+00   0.321E+01
  0.1562E+00   0.467E+02   0.000E+00   0.151E+02   0.479E-01   0.655E-01   0.179E+00   0.277E+01
  0.1875E+00   0.472E+02   0.000E+00   0.166E+02   0.431E-01   0.654E-01   0.174E+00   0.255E+01
  0.2187E+00   0.459E+02   0.000E+00   0.180E+02   0.407E-01   0.657E-01   0.172E+00   0.234E+01
  0.2500E+00   0.478E+02   0.000E+00   0.194E+02   0.353E-01   0.630E-01   0.161E+00   0.213E+01
  0.2812E+00   0.489E+02   0.000E+00   0.210E+02   0.345E-01   0.638E-01   0.162E+00   0.199E+01
  0.3125E+00   0.473E+02   0.000E+00   0.225E+02   0.326E-01   0.668E-01   0.166E+00   0.205E+01
  0.3437E+00   0.481E+02   0.000E+00   0.240E+02   0.311E-01   0.648E-01   0.161E+00   0.186E+01
  0.3750E+00   0.470E+02   0.000E+00   0.255E+02   0.301E-01   0.662E-01   0.163E+00   0.184E+01
  0.4062E+00   0.499E+02   0.000E+00   0.269E+02   0.300E-01   0.650E-01   0.160E+00   0.167E+01
  0.4375E+00   0.461E+02   0.000E+00   0.285E+02   0.297E-01   0.667E-01   0.163E+00   0.166E+01
  0.4687E+00   0.375E+02   0.000E+00   0.298E+02   0.287E-01   0.660E-01   0.161E+00   0.157E+01
  0.5000E+00   0.305E+02   0.000E+00   0.309E+02   0.282E-01   0.653E-01   0.159E+00   0.148E+01
  0.5312E+00   0.157E+02   0.000E+00   0.316E+02   0.281E-01   0.632E-01   0.155E+00   0.132E+01
  0.5625E+00   0.546E+01   0.000E+00   0.319E+02   0.280E-01   0.649E-01   0.158E+00   0.126E+01
  0.5937E+00   0.241E+01   0.000E+00   0.320E+02   0.284E-01   0.614E-01   0.151E+00   0.108E+01
  0.6250E+00   0.170E+00   0.000E+00   0.321E+02   0.315E-01   0.619E-01   0.155E+00   0.995E+00